Table A1.

Spectral parameters of the SSsed model.

Description
par1Mass, black hole mass in solar masses
par2Dist, comoving (proper) distance in kpc
par3|$\log \dot{m}$|⁠, |$\dot{m}=\dot{M}/\dot{M}_{\rm Edd}$| where |$\dot{M}_{\rm Edd}c^2=L_{\rm Edd}$|
par4rin, inner most radius of the accretion flow in rg
par5cos i, inclination angle of the disc
par6kTe, th, electron temperature for thermal corona in keV. If this parameter is negative, the model gives the inner hot Comptonization component.
par7kTe, nth, apparent electron temperature for non-thermal corona in keV which is recommended to be fixed at 300 keV to mimic non-thermal electron distribution. If this parameter is negative, the model gives the Comptonization component in the passive-disc corona region.
par8Γth, photon index of inner hot corona. If this parameter is negative then only the inner Compton component is used.
par9Γnth, photon index of disc-corona. If this parameter is negative, the model gives the outer disc.
par10fth, fraction of the hot Comptonizing component to the total Comptonization
par11rcor, outer radius of the disc-corona region in rg
par12log rout, outer radius of accretion disc in rg. If this parameter is −1, the code will use the self gravity radius as calculated from Laor & Netzer (1989)
par13redshift, must be fixed
par14fcol, switching parameter for colour correction (0: no colour correction, 1: colour correction factor is calculated by the same way as optxagnf (Done et al. 2012)
par15norm, must be fixed at 1
Description
par1Mass, black hole mass in solar masses
par2Dist, comoving (proper) distance in kpc
par3|$\log \dot{m}$|⁠, |$\dot{m}=\dot{M}/\dot{M}_{\rm Edd}$| where |$\dot{M}_{\rm Edd}c^2=L_{\rm Edd}$|
par4rin, inner most radius of the accretion flow in rg
par5cos i, inclination angle of the disc
par6kTe, th, electron temperature for thermal corona in keV. If this parameter is negative, the model gives the inner hot Comptonization component.
par7kTe, nth, apparent electron temperature for non-thermal corona in keV which is recommended to be fixed at 300 keV to mimic non-thermal electron distribution. If this parameter is negative, the model gives the Comptonization component in the passive-disc corona region.
par8Γth, photon index of inner hot corona. If this parameter is negative then only the inner Compton component is used.
par9Γnth, photon index of disc-corona. If this parameter is negative, the model gives the outer disc.
par10fth, fraction of the hot Comptonizing component to the total Comptonization
par11rcor, outer radius of the disc-corona region in rg
par12log rout, outer radius of accretion disc in rg. If this parameter is −1, the code will use the self gravity radius as calculated from Laor & Netzer (1989)
par13redshift, must be fixed
par14fcol, switching parameter for colour correction (0: no colour correction, 1: colour correction factor is calculated by the same way as optxagnf (Done et al. 2012)
par15norm, must be fixed at 1
Table A1.

Spectral parameters of the SSsed model.

Description
par1Mass, black hole mass in solar masses
par2Dist, comoving (proper) distance in kpc
par3|$\log \dot{m}$|⁠, |$\dot{m}=\dot{M}/\dot{M}_{\rm Edd}$| where |$\dot{M}_{\rm Edd}c^2=L_{\rm Edd}$|
par4rin, inner most radius of the accretion flow in rg
par5cos i, inclination angle of the disc
par6kTe, th, electron temperature for thermal corona in keV. If this parameter is negative, the model gives the inner hot Comptonization component.
par7kTe, nth, apparent electron temperature for non-thermal corona in keV which is recommended to be fixed at 300 keV to mimic non-thermal electron distribution. If this parameter is negative, the model gives the Comptonization component in the passive-disc corona region.
par8Γth, photon index of inner hot corona. If this parameter is negative then only the inner Compton component is used.
par9Γnth, photon index of disc-corona. If this parameter is negative, the model gives the outer disc.
par10fth, fraction of the hot Comptonizing component to the total Comptonization
par11rcor, outer radius of the disc-corona region in rg
par12log rout, outer radius of accretion disc in rg. If this parameter is −1, the code will use the self gravity radius as calculated from Laor & Netzer (1989)
par13redshift, must be fixed
par14fcol, switching parameter for colour correction (0: no colour correction, 1: colour correction factor is calculated by the same way as optxagnf (Done et al. 2012)
par15norm, must be fixed at 1
Description
par1Mass, black hole mass in solar masses
par2Dist, comoving (proper) distance in kpc
par3|$\log \dot{m}$|⁠, |$\dot{m}=\dot{M}/\dot{M}_{\rm Edd}$| where |$\dot{M}_{\rm Edd}c^2=L_{\rm Edd}$|
par4rin, inner most radius of the accretion flow in rg
par5cos i, inclination angle of the disc
par6kTe, th, electron temperature for thermal corona in keV. If this parameter is negative, the model gives the inner hot Comptonization component.
par7kTe, nth, apparent electron temperature for non-thermal corona in keV which is recommended to be fixed at 300 keV to mimic non-thermal electron distribution. If this parameter is negative, the model gives the Comptonization component in the passive-disc corona region.
par8Γth, photon index of inner hot corona. If this parameter is negative then only the inner Compton component is used.
par9Γnth, photon index of disc-corona. If this parameter is negative, the model gives the outer disc.
par10fth, fraction of the hot Comptonizing component to the total Comptonization
par11rcor, outer radius of the disc-corona region in rg
par12log rout, outer radius of accretion disc in rg. If this parameter is −1, the code will use the self gravity radius as calculated from Laor & Netzer (1989)
par13redshift, must be fixed
par14fcol, switching parameter for colour correction (0: no colour correction, 1: colour correction factor is calculated by the same way as optxagnf (Done et al. 2012)
par15norm, must be fixed at 1
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